Epstein-Glaser’s causal light-front field theory
Autor(a) principal: | |
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Data de Publicação: | 2019 |
Outros Autores: | , |
Tipo de documento: | Artigo de conferência |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UNESP |
Texto Completo: | http://hdl.handle.net/11449/200571 |
Resumo: | Epstein-Glaser’s ideas for the formulation of a distributional well-defined perturbative causal field theory are developed in light-front dynamics over the invariant null-plane coordinates introduced by Rohrlich. Explicitly, the causality theorems which warrant the method are adapted to that dynamics, and the causal distribution splitting formulae are re-derived in accordance with it, exhibiting important differences with respect to its instant dynamics version. Application of these splitting formulae to the (anti)commutation relations of the fermion and radiation fields naturally leads to the well known instantaneous terms of their Feynman propagators, while the scalar field’s one retains its form from instant dynamics. Additionally, the developed method is applied to Scalar QED (SQED) at second order, taking for the first order distribution the product of the radiation field with only the linear in the coupling constant part of the current. We analyse Moeller scattering, for which the equivalence with instant dynamics is established, and Compton scattering, for which the vertex coming from the second order term in the current is automatically generated in the normalization procedure once the residual gauge invariance which remains from the imposition of the null-plane gauge condition is exploited. |
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Epstein-Glaser’s causal light-front field theoryEpstein-Glaser’s ideas for the formulation of a distributional well-defined perturbative causal field theory are developed in light-front dynamics over the invariant null-plane coordinates introduced by Rohrlich. Explicitly, the causality theorems which warrant the method are adapted to that dynamics, and the causal distribution splitting formulae are re-derived in accordance with it, exhibiting important differences with respect to its instant dynamics version. Application of these splitting formulae to the (anti)commutation relations of the fermion and radiation fields naturally leads to the well known instantaneous terms of their Feynman propagators, while the scalar field’s one retains its form from instant dynamics. Additionally, the developed method is applied to Scalar QED (SQED) at second order, taking for the first order distribution the product of the radiation field with only the linear in the coupling constant part of the current. We analyse Moeller scattering, for which the equivalence with instant dynamics is established, and Compton scattering, for which the vertex coming from the second order term in the current is automatically generated in the normalization procedure once the residual gauge invariance which remains from the imposition of the null-plane gauge condition is exploited.Instituto de Física Teórica (IFT) Universidade Estadual Paulista (UNESP) R. Dr. Bento, Teobaldo Ferraz 271Facultad de Ciencias Universidad Nacional de Ingeniería (UNI), Avenida Túpac Amaru S/N apartadoInstituto de Física Teórica (IFT) Universidade Estadual Paulista (UNESP) R. Dr. Bento, Teobaldo Ferraz 271Universidade Estadual Paulista (Unesp)Universidad Nacional de Ingeniería (UNI)Acevedo, O. A. [UNESP]Pimentel, B. M. [UNESP]Soto, D. E.2020-12-12T02:10:06Z2020-12-12T02:10:06Z2019-01-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/conferenceObjectProceedings of Science, v. 374.1824-8039http://hdl.handle.net/11449/2005712-s2.0-85085998658Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengProceedings of Scienceinfo:eu-repo/semantics/openAccess2021-10-23T14:47:55Zoai:repositorio.unesp.br:11449/200571Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T17:09:40.640353Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false |
dc.title.none.fl_str_mv |
Epstein-Glaser’s causal light-front field theory |
title |
Epstein-Glaser’s causal light-front field theory |
spellingShingle |
Epstein-Glaser’s causal light-front field theory Acevedo, O. A. [UNESP] |
title_short |
Epstein-Glaser’s causal light-front field theory |
title_full |
Epstein-Glaser’s causal light-front field theory |
title_fullStr |
Epstein-Glaser’s causal light-front field theory |
title_full_unstemmed |
Epstein-Glaser’s causal light-front field theory |
title_sort |
Epstein-Glaser’s causal light-front field theory |
author |
Acevedo, O. A. [UNESP] |
author_facet |
Acevedo, O. A. [UNESP] Pimentel, B. M. [UNESP] Soto, D. E. |
author_role |
author |
author2 |
Pimentel, B. M. [UNESP] Soto, D. E. |
author2_role |
author author |
dc.contributor.none.fl_str_mv |
Universidade Estadual Paulista (Unesp) Universidad Nacional de Ingeniería (UNI) |
dc.contributor.author.fl_str_mv |
Acevedo, O. A. [UNESP] Pimentel, B. M. [UNESP] Soto, D. E. |
description |
Epstein-Glaser’s ideas for the formulation of a distributional well-defined perturbative causal field theory are developed in light-front dynamics over the invariant null-plane coordinates introduced by Rohrlich. Explicitly, the causality theorems which warrant the method are adapted to that dynamics, and the causal distribution splitting formulae are re-derived in accordance with it, exhibiting important differences with respect to its instant dynamics version. Application of these splitting formulae to the (anti)commutation relations of the fermion and radiation fields naturally leads to the well known instantaneous terms of their Feynman propagators, while the scalar field’s one retains its form from instant dynamics. Additionally, the developed method is applied to Scalar QED (SQED) at second order, taking for the first order distribution the product of the radiation field with only the linear in the coupling constant part of the current. We analyse Moeller scattering, for which the equivalence with instant dynamics is established, and Compton scattering, for which the vertex coming from the second order term in the current is automatically generated in the normalization procedure once the residual gauge invariance which remains from the imposition of the null-plane gauge condition is exploited. |
publishDate |
2019 |
dc.date.none.fl_str_mv |
2019-01-01 2020-12-12T02:10:06Z 2020-12-12T02:10:06Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/conferenceObject |
format |
conferenceObject |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
Proceedings of Science, v. 374. 1824-8039 http://hdl.handle.net/11449/200571 2-s2.0-85085998658 |
identifier_str_mv |
Proceedings of Science, v. 374. 1824-8039 2-s2.0-85085998658 |
url |
http://hdl.handle.net/11449/200571 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
Proceedings of Science |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.source.none.fl_str_mv |
Scopus reponame:Repositório Institucional da UNESP instname:Universidade Estadual Paulista (UNESP) instacron:UNESP |
instname_str |
Universidade Estadual Paulista (UNESP) |
instacron_str |
UNESP |
institution |
UNESP |
reponame_str |
Repositório Institucional da UNESP |
collection |
Repositório Institucional da UNESP |
repository.name.fl_str_mv |
Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP) |
repository.mail.fl_str_mv |
|
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1808128763856158720 |